IRJET- Analysis of Tuned Liquid Damper (TLD) in Controlling Earthquake Response of a Building using

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Analysis of Tuned Liquid Damper (TLD) in Controlling Earthquake Response of a Building using SAP2000 Mr. Aakash Bikram Rana1, Mr. Shubhesh Bista2, Mr. Prashant Sunagar3 1,2Alumni,

Dept. Of Civil Engineering, Ramaiah Institute of Technology, Karnataka, India Professor, Dept. Of Civil Engineering, Ramaiah Institute of Technology, Karnataka, India --------------------------------------------------------------------------***----------------------------------------------------------------------3Asst.

Abstract - This project aims to study the effectiveness of Tuned Liquid Dampers (TLD) in reducing the seismic vibration of a building when it is subjected to horizontal sinusoidal excitation. TLD is a water confined container, or simply a water tank, which uses the sloshing energy of water to reduce the dynamic response of a structure when it is subjected to excitation. In this study, a procedure for designing TLD for a building is suggested and a method is proposed to model the TLD in SAP2000 software. Then, multiple analyses have been carried out to analyse the effect of different parameters of TLD which may affect its performance. Analyses are conducted with varying mass ratio, tuning ratio, excitation ratio, number of storeys, position of TLD, etc. The structural response is compared based on maximum base shear, maximum relative acceleration and maximum displacement of top storey. With reference to the results from these analyses, conclusions are derived and recommendations are given for an optimal design of TLD. Keywords: Tuned Liquid Damper, SAP2000, Earthquake Engineering, Modelling, Dampers, TLD

1

INTRODUCTION:

Earthquakes are perhaps the most disastrous and unpredictable among all the natural calamities. We have witnessed many high intensity earthquakes which have claimed numerous lives and have damaged an immeasurable amount of properties. They not only pose a threat to humans but also have a tremendous impact on the surrounding including the structures. In such cases where the structures lie in an earthquake prone area, the designers, architects and engineers have to take adequate precautions to safeguard the structures against the effect of earthquake. Many techniques are available to reduce the effect of earthquake on structures. This paper discusses and analyses the applicability of tuned liquid damper in reducing the earthquake effect on building.

1.1

Tuned Liquid Dampers (TLD)

When earthquake forces hit a structure it imparts energy to it which causes vibration, If by any means we can absorb the imparted energy, we can easily reduce the amplitude of vibration of the building. This is usually termed as “damping”. One way of doing this is by facilitating the structure with a “Tuned Liquid Damper (TLD)”. It was first introduced in the 1980s

by Bauer and later installed in several other buildings, the recent being One Rincon Hill tower of San Francisco.

TLDs are basically a tank partially filled with water or sometimes with sugar solution usually installed on the top of the building. Buildings under earthquake forces starts vibrating at a particular frequency called natural frequency, TLDs are designed to have the same natural frequency so that sloshing of liquid in the tank under external excitation generates antiphase to the building motion as shown in figure 1.

TLD acts as a passive energy dissipation device and has following advantages over other damping systems

Figure 1.1: Principle of TLD working

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Low cost - installation as well as maintenance Easy installation in new as well as in existing buildings Non restriction to unidirectional vibration Easily adjustable natural frequency of the tank by simply adjusting the water depth.

Water in tanks can be utilized during emergency such as during fire hazards.

Based on depth of water, shape and function, TLDs are classified into following categories: TSD: Tuned Sloshing Damper; TLCD: Tuned Liquid Column Damper; LCVA: Liquid Column Vibration Absorber; DTLCD: Double Tuned Liquid Column Damper; HTLCD: Hybrid Tuned Liquid Column Damper; PTLCD: Pressurized Tuned Liquid Column Damper

1.2

Parameters affecting the behaviour of TLD

There are different parameters that affect the behaviour of TLD in building. These are natural frequency of building, excitation frequency ratio, mass ratio, depth ratio, tuning frequency ratio, shape of the tank and position of the tank on the building. All these are explained below.

Tuning ratio: Tuning ratio is the ratio of frequency of TLD to the frequency of the building. The damping effect of TLD is best when tuning ratio is 1, and is known to reduce sharply as it moves away from unity.

Mass ratio: Mass ratio is the ratio of the mass of the liquid in TLD to the mass of the building. The effect of damping often increases with the increase in mass ratio. This is because the increase in mass will mean the TLD will have more damping force or sloshing force to counter the earthquake force.

Depth ratio: Depth ratio is the ratio of the depth of the tank to the length of the tank in the direction of sloshing. Water mass may be divided into convective mass and impulsive mass out of which convective mass has the participation in sloshing mechanism. The ratio of convective mass to impulsive mass of water is inversely related to the depth ratio. So, higher depth ratio would mean lesser convective mass and thence, lesser participation in sloshing. Hence, a lower depth ratio is often preferred.

Shape of tank: The shape of the tank can be circular, rectangular, conical or geometrical shape. Different shape of tank depicts different sloshing behaviour. Often, it is the rectangular tank or circular tank that is used because of its simplicity.

Even in design codes, such as IS1893:2002 part 2, the charts are available only for circular and rectangular tanks, so they are more preferred for the analysis purpose.

Position of tank: Position of the tank also affects the behaviour of the TLD. The position of TLD can be in some mid storey or somewhere at the top of building. The position can also be at the centre, edge or at the corner of the storey in which it is placed. Most literature shows that the best effect of TLD is obtained when it is placed on the terrace.

Figure 1.2: Types of TLD

2

LITERATUREREVIEW

Till date, TLD has been studied by several researchers. Some of them are given below.

(Soong, T.T; Dargush, Gary F., 1997) Provides reviews on the theoretical studies done on TLD system and various experiments conducted on different TLD designs. Factors controlling various design parameters are introduced.

Comparative studies made on these factors were made to find optimum designs. Integration of different materials in buildings constructed are introduced and their performance statistics are shown. This book provides, for the first time, an © 2018, IRJET

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extensive exploration of the various types of energy dissipation that are currently available to structural designers. The book starts with a short chapter on structural dynamics and then goes straight into chapters that provide detailed discussions of various damping systems. All the standard damping systems are included such as "Metallic Dampers", "Friction Dampers", "Viscoelastic Dampers", "Viscous Fluid Dampers", "Tuned Mass Dampers" and "Tuned Liquid Dampers", and the book also includes a chapter on the more esoteric topic of "Smart Materials" which outlines how some innovative materials can be incorporated into damping elements (Bauer, H. F., 1984) Was amongst the first researchers who applied TLDs to ground civil engineering structures by introducing a rectangular tank full of two immiscible liquids to decrease structural vibration. （K. Fujii, Y. Tamura, T. Sato, T. Wakahara，1990） Found that wind-induced vibrations of two buildings in Nagasaki and Yokohama, were reduced to about half upon installation of Tuned Sloshing Damper.

Wakahara carried out theoretical and experimental studies to design an optimum TLD and verified the TLD with a project in Yokohama. The interaction model considered by them was based on the Boundary Element Method for simulating liquid motion in a TLD container, and Multi-degrees of Freedom for the structure method. The TLD installation on the building could reduce the wind-induced response up to half the original value.

Tamura found that the damping ratio of 77.6m high Tokyo international Airport Tower increased to 7.6% from 1.0% by using Tuned liquid Damper.

(L.M. Sun, Y. Fujino, B.M.Pacheco , and P. Chaiseri, 1992) Explained a nonlinear model for rectangular Tuned Liquid Damper. This model utilizes shallow water wave theory with consideration of liquid damping effects. The model is further extended to account for the effect of breaking waves. Two empirical coefficients were identified experimentally and are introduced in the model. It was then experimentally verified that the model can well predict the response of structures installed with TLD's even when breaking waves occur.

(V.J. Modi, S.R. Munshi, 1998) Introduced a semi-circular obstacle in the damper to accelerate and enhance the liquid sloshing and to increase the energy dissipation. They conducted an experimental study to improve the TLD efficiency by introducing a two-dimensional obstacle. Then, they conducted a parametric study to obtain the optimum size and location of the obstacle. As per the results, up to 60% increase in energy dissipation was observed in the presence of the obstacle. （F. Casciati, A.D. Stefano, E. Matta，2003）Studied the use of frustum-conical TLD as an alternative to the traditional cylindrical tank. A linear model is presented which can interpret TLD's behaviour for small excitations. However, for larger amplitudes, the linear model is no longer valid because strong nonlinearities exist. Furthermore, to represent the frustum-cone TLD subjected to harmonic excitations, a tuned mass damper (TMD) analogy is established where TMD parameters vary with the excitation amplitude. （Kim Y.M., You K.P., Cho J.E., Hong D.P.，2006）Conducted shake table experiments to investigate the characteristics of water sloshing motion in TLD (rectangular and circular) and TLCD. They found the parameters such as wave height, base shear force, and energy dissipation etc. from the experiment. It was found that the TLCD was more effective in controlling vibration than TLD. （Shang C.Y., Zhao J.C.，2008）Presented a novel tuned liquid damper (TLD) rectangular tank with two angle-adjustable baffles. The numerical analysis was performed using the commercial code FLUENT. The standard kinetic energy and dissipation rate turbulent model was employed, which was solved using volume of fluid (VOF) method able to treat both the free surface motion and the viscous stresses over the rigid walls accurately. The relationship between the natural periods of water and the angles of its baffles was studied by numerical simulating of a case, and the changes of energy dissipations were investigated. The natural periods and dampers of the novel TLD can be changed in a wide range by adjusting the baffles’ angle, thus it is more effective in controlling the vibration of structures in a wide frequency range. （X.L. Xu, K.C.S. Kwok, B. Samali，1992）Made an investigation on the possible application of tuned liquid column dampers (TLCD) and tuned liquid column/mass dampers (TLCMD) in reducing the cross-wind response of wind sensitive structures. The structure is modelled as a lumped mass multi-degree freedom system taking into account both bending and shears. The cross-wind wake excitation is modelled as a stochastic process which is stationary in time and nonhomogeneous in space. A random vibration analysis utilising transfer matrix formulation is carried out to obtain response statistics. The non-linear damping term in the fundamental equation of the tuned liquid damper is treated by an equivalent linear technique. Numerical examples show that tuned liquid dampers, which have significant practical advantages, can © 2018, IRJET

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achieve the same motion reduction level as the traditional tuned mass dampers if the parameters of the liquid dampers are properly selected. However, excessive liquid motion in a tuned liquid column/mass damper may reduce the effectiveness of this damper and therefore a careful selection of the frequency tuning ratios of the damper is necessary. （Samanta A., Banerji P.，2008）Designed a modified configuration of TL, in which the liquid tank, instead of being rigidly connected to the floor, was elevated using an appropriately designed torsion spring. Greater effectiveness was observed.

(Housner G. W., 1963) was the person to develop spring mass analogy for modelling water tanks. Here, we can find the formulas for calculating different parameters of the spring mass system like convective mass, impulsive mass and their respective heights like convective height and impulsive heights. He has done analytical analysis of TLD of rectangular as well as circular cross sections. Later, his work was adopted in building the IS1893 part 2 which is related to the earthquake resistant design of water tanks situated at ground as well as elevated circular and rectangular tanks.

(N.S. Sebastian, 2017) Modelled water tank in two parts namely convective mass and impulsive mass. The convective mass acts as a sloshing mass of water which is present above the impulsive mass which acts as fixed mass of water tank at the bottom portion. He has modelled the water tank using the mass spring system. He has done a linear static analysis and time history analysis of a framed structure. The buildings used were 3, 6, 9 and 12 storey buildings. He found 64% reduction in 3 storey building and 84% in 12 storey building. He found it increasing with increase in number of storey. He compared the results with tank and without tank and shape of tank being circular as well as rectangular.

(T. Novo, H. Varum, F. Teixeira-Dias, H. Rodrigues, M. Falcao Silva, A. Campos Costa, L. Guerreiro, 2013) Studied the behaviour of an isolated TLD, subjected to a sinusoidal excitation at its base, with different displacement amplitudes by finite element method. He concluded that for a sinusoidal cyclic loading, the behaviour of the TLD is globally efficient, significantly increasing the energy dissipation and causing a corresponding equivalent damping of the global system. The TLD is highly effective in reducing the structural demand for structures with a low natural period.

3

OBJECTIVE AND SCOPE:

The objective of this study is to develop a model of Tuned Liquid damper in SAP2000 and to carry out multiple analyses on it. In summary, the scope and objectives of this study can be listed out as follows:    

Modelling of a structure with TLD in SAP2000 and analysing the effect of TLD on the structure Re-affirming the different parameters of TLD which affects its performance and thus giving recommendations on it – mass ratio, depth ratio, excitation ratio and tuning ratio.

Comparing the effect of TLD for buildings of different storeys / height.

Study the effects of TLD on the building when it is placed at different locations on the terrace.

4

METHODOLOGY:

The entire procedure of making the model and conducting the analysis is broken down into a set of steps as given below.

1 2 3 4

Modelling of the structure using SAP2000 Designing the TLD for structure Modelling of the TLD using SAP2000 Analysis

The set of steps used for designing and modelling structure and TLD is explained in this section using an example of a 20 storey building. Then, similar procedure was used for all other buildings used in the analysis and then the results were compared.

4.1

Modelling of the structure using SAP2000

First, the given structure is modelled in SAP2000. For this analysis, a simple 20 storey RC bare frame is considered with properties as given below.

4.1.1

Properties of the RC frame

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Number of grid lines in Y direction = 6 Number of grid lines in Z direction = 21 Spacing in X direction = 4m Spacing in Y direction = 4m Spacing in Z direction = 3.5m 4.1.2

Defining material Properties

M50 concrete of Indian standard is defined.

HYSD rebars of Fe500 is defined.

4.1.3

Defining the frame sections

Column size of 0.6mX0.6m of M50 grade using Fe500 rebars is used.

Beam size of 0.6mX0.3m of M50 grade using Fe500 rebars is used.

4.1.4

Defining the slab section

The slab of 250 mm thickness of M30 material is used for modelling of a structure.

4.1.5

Assigning the support condition:

The base of the building in the plan the xy plane view is selected and fixed support condition was assigned.

4.1.6

Defining Load Pattern

Dead load, Live load (4 kN/m2), other load (Floor finish and Partition load = 2 kN/m 2) and earthquake load of zone 5 with soil type II and 5 % damping confirming to IS1893:2002 with 1 scale factor.

4.1.7

Defining Time History Function

We used time history Sine function for the Time History Analysis. The time period of the function was made same as that of the building to have the maximum effect of earthquake on the structure. The scale factor used is ZIS a/2R. So, for ordinary RC frame building of zone 5 in soft soil, scale factor with be: 0.36*1*(1.67/2)/2/3*9.81 = 0.491. It can be seen in the figures 4.1 and 4.2.

Figure 4.1: Defining sinusoidal time history function Š 2018, IRJET

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Figure 4.2: Defining sinusoidal time history load case 4.2 Designing the TLD for the structure The TLD is designed such that its frequency is slightly lower than the fundamental frequency of the building under consideration. Here, the TLD is modelled as a spring mass system as specified in IS1893:2002 Indian code. The design curves present in the IS code are used for the design purpose. The steps for design are outlined below.

4.2.1 Selecting design parameters Mass ratio (mr = 2%) Depth ratio (dr = .2) Mass of building (M’ = 9425200kg) Fundamental frequency of the building (f’ = .5Hz) Maximum length of TLD specified for the building (L’ = 12m) 4.2.2 Obtaining optimal tuning frequency It is given by: f = f’/(1+mr) = .49Hz 4.2.3 Using IS 1893:2002 part 2 curves For the given depth ratio, dr = 0.2, we can obtain, mc/m = .77 hi/h = 2 mi/m = .23 hc/h = 2.8 Kh/mg = .25 4.2.4 Obtaining dimension of each tank Frequency of spring is given by: f=1/2π*√(k/mc) Putting values of k and mc from IS curves, we get, © 2018, IRJET

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f = 1/2π*√((.25*mg/h)/(.77m)) So,

h = 1/(2πf)2*.25g/.77 = .336m

Length of liquid = L = h/depth ratio = .131/.2 = 1.679m Maximum height of sloshing can be obtained by IS code as: hs = Ah*R*L/2 = (ZISa/2Rg)*R*L/2 = .075*2*1.679/2 = .126m So, inner height of tank required = h + hs = .336+.126 = .462m Assuming 150mm wall thickness,

Figure 4.3: Spring mass analogy for TLD Therefore, Size of each tank = 1.979mX1.979mX.612 m

Figure 4.4: IS curves for parameters of the spring mass model for rectangular tank 4.2.5 Finding the number and arrangement of TLDs Mass of each tank m = L2h*1000 = 946kg Number of tanks required, n = mr*M’/m = .02*9425200/946 = 200 © 2018, IRJET

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If L’ = 12m length is given as TLD space in terrace, then, Number of TLDs in each direction = 12/1.979= 15.9 = 6 no.

And, number of TLD layers required = 200/6/6 = 6 no Hence, no of TLDs provided = 6*6*6= 216 4.2.6 Obtaining parameters for each spring mass system Mass of liquid in each tank, m = 1000*L2*h = 55.6kg mc/m = .77 => mc = .77*946 = 728kg mi/m = .23; 77 => mi = .23*946 = 218kg Kh/mg = .25 => K = .25*946*9.8/.336 = 6904N/m hc/h = 2.8 => hc = 2.8*946 = .94m hi/h = 2 => hi = 2*946= .672m 4.2.7 Modelling the set of spring mass systems as a single equivalent spring mass system The number of TLDs in each building is a very high number and modelling each one of them will be a tedious and an impractical task. So, in order to simplify the analysis, it is more intuitive to model the set of TLDs as a single equivalent spring mass system.

If ‘n’ be the no of TLDs in the entire system, the equivalent parameters for the equivalent system can be obtained as follows.

If ‘f’ be force applied by each tank then for ‘n’ tanks, the total force applied is nf. Let ‘F’ be equivalent force applied by the equivalent system. Let small letters k, m and h represent stiffness, masses and heights for each tank and capital letters K, M, and H represent corresponding parameters for the equivalent system. Then, here, F = nf Kx+Ma = n(kx+ma) Kx+Ma=nkx+nma Equating coefficients of x and a, K = n*k = 1381kN/m M = n*m = 189200kg Similarly, we can write, Mi = n*mi = 43527kg Mc=n*mc = 145719kg Height values can be obtained as the average height value of all the layers about the bottom. After simplifying, we get, Hi = hi+ (no of layers-1)*height of tank/2 = 1.49m Hc = hc+ (no of layers-1)*height of tank/2 = 1.76m

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4.3 Modelling of the TLD using SAP2000 Tank frame is modelled using columns of same size as that of building which is then in filled with concrete wall panels.

Spring for convective mass is modelled using “linear link” element whose stiffness in X and Y direction is given as K/2 and its DOF in Z direction is set as fixed. Spring for impulsive mass is also modelled using linear link element, but its DOF is set fixed in all direction.

“Joint mass” is assigned at the joint of the spring with values Mc and Mi in X and Y direction.

“Joint force” is assigned at the joint of the spring with values M c and Mi in GRAVITY direction.

Figure 4.8: TLD model in the structure

Figure 4.7: Assigning link properties to model TLD

Figure 4.6: Assigning joint masses

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Figure 4.6: Assigning joint load

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4.4 Analysis The analysis was carried out by considering different parameters to understand the behaviour of TLD. A standard G+19 storey building with TLD was modelled and it was tested with different excitation frequency ratios, different depth ratio, different locations of TLD on the terrace and different mass ratios. While analysing one particular parameter, the other parameters and other components of the building were kept constant.

The tuning frequency of the building is the ratio of frequency of TLD to the frequency of the building. Tuning ratio was varied from 0.8 to 1.2 and analysis was done for the different tuning ratios Depth ratio is the depth of water in TLD to the length of liquid in sloshing direction. The depth ratio was varied from 0.1 to 0.5 and comparative analysis was carried out.

Effect of TLD when placed at different locations of the terrace was analysed. The different locations on terrace considered in the study were centre, edge and corner.

The mass ratio is the ratio of mass of TLD to the mass of the building. The mass ratios varying from 1% to 5% were analysed.

The analysis for different storeys of building was also done. The number of storeys was varied from 10 storeys to 35 storeys.

The results were analysed on the basis of percentage reduction in maximum displacement and acceleration of a joint in the top storey of the building along with percentage reduction in base shear force after the implementation of TLD. The analysis carried out was time history analysis using sinusoidal wave whose peak acceleration was obtained from the equation given in IS code, given as ZISa/2R in m/s2.

5

RESULTS:

The results obtained are given below under various topics.       

Standard TLD designed for a G+19 building TLDs at different excitation frequency ratios TLDs with different tuning ratios TLDs with different depth ratios TLDs with different mass ratios TLDs at different locations on the terrace TLDs for different number of storeys of building

5.1 Standard TLD designed for a G+19 building Table 5.1: Results for Time History analysis for sine wave with time period same as time period of the structure

Maxm joint accln in top storey without TLD

Units m/s2

Values 4.945

Maximum joint displacement in top storey without TLD

m

0.5252

Base shear without TLD

kN

37434

Maximum joint accln in top storey with TLD

m/s2

2.915

Maximum joint displacement in top storey with TLD

m

0.2979

Base shear with TLD

kN

22140

% reduction in relative acceleration

%

41.100

% reduction in displacement

%

43.279

% reduction in base shear © 2018, IRJET

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Table 5.2: Results for Response Spectrum analysis

Maxm joint accln in top storey without TLD Maximum joint displacement in top storey without TLD Base shear without TLD Maximum joint accln in top storey with TLD Maximum joint displacement in top storey with TLD Base shear with TLD % reduction in relative acceleration % reduction in displacement % reduction in base shear

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Units m/s2 m kN m/s2 m kN %

Values 0.6561 0.04116 3409 0.592 0.0335 2892 9.770

%

18.610 15.166

%

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5.2 XTLDs at different excitation frequency ratio Table 5.2: Results for different excitation frequency ratios Without TLD Acceleration Displacement

Excitation ratio

Base shear

4.00 2.00 1.25 1.11 1.00 0.91 0.83 0.67 0.50 0.40

2171.574 8619.194 12677.107 23693.538 37434 30633.855 21924.432 12790.042 9019.358 8619.194

0.53375 0.37471 2.47338 3.86512 4.945 3.34837 2.12303 0.8883 0.52469 0.37471

0.019018 0.083142 0.197561 0.338255 0.525 0.395662 0.26978 0.161546 0.099356 0.083142

Base shear 2260.101 8568.755 11821.74 19151.79 4 22140 21776.76 9 22487.33 6 12664.67 7 8960.604 8568.755

With TLD Acceleration

Displacement

0.54466 0.36254 2.28712 3.16936 2.195 2.38013 2.15143 0.80837 0.51361 0.36254

0.017815 0.083834 0.172095 0.27269 0.2979 0.305505 0.311321 0.161645 0.105082 0.083834

5.3 TLDs with different tuning ratios Table 5.3 Results for different tuning ratio Tuning ratio Maxm accln without TLD Maxm disp. without TLD Base shear without TLD Maxm accln with TLD Maxm disp. with TLD Base shear with TLD % reduction in accln © 2018, IRJET

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0.800

0.900

0.950

0.975

1.000

1.025

1.050

1.100

1.200

4.955

4.957

4.902

4.958

4.958

4.948

4.866

4.935

4.864

0.5252

0.5259

0.5247

0.523

0.525

0.527

0.5223

0.526

0.5222

37483

37488

37450

37300

3747

37570

37325

37508

37326

4.289

3.478

3.024

2.937

2.877

2.849

2.895

3.265

4.15

0.456

0.3533

0.3018

0.298

0.298

0.2996

0.3058

0.3411

0.411

33203

26846

23038

22128

2191

21882

21859

24058

30345

13.441

29.837

38.311

40.762

41.97

42.421

40.506

33.840

14.679

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13.176

32.820

42.481

43.021

43.27

43.150

41.451

35.152

21.295

11.419

28.388

38.483

40.676

41.50

41.757

41.436

35.859

18.703

5.4 TLDs with different depth ratios Table 5.4: Results for different depth ratio Depth ratio Maxm joint accln without TLD Maximum displacement without TLD

0.10 4.872 0.495

0.20 4.945 0.5252

0.30 4.957 0.5258

0.40 4.953 0.5255

0.50 4.958 0.5233

Base shear without TLD Maximum accln with TLD Maximum displacement with TLD

37411 2.702 0.2852

37434 2.195 0.2979

37471 3.107 0.3132

37495 3.119 0.3139

37306 3.426 0.3478

Base shear with TLD % reduction in relative acceleration

20898 44.540

22140 55.612

23546 37.321

23601 37.028

25761 30.900

% reduction in displacement % reduction in base shear

42.384 44.139

43.279 40.856

40.434 37.162

40.266 37.056

33.537 30.947

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5.5 TLDs with different mass ratios Table 5.5: Results of different mass ratio Mass ratio Maxm joint accln without TLD Maximum displacement without TLD Base shear without TLD Maximum accln with TLD Maximum displacement with TLD Base shear with TLD % reduction in relative acceleration % reduction in displacement % reduction in base shear

1.0% 4.98 0.514 36879 3.716 0.363 27430 25.382 29.377 25.622

1.5% 4.895 0.522 37566 3.189 0.323 24650 34.852 38.123 34.382

2.0% 5 0.53 37426 2.38 0.301 21701 52.400 43.208 42.016

2.5% 4.956 0.526 37419 2.696 0.276 20596 45.601 47.529 44.958

3.0% 4.821 0.509 37006 2.416 0.238 18547 49.886 53.242 49.881

5.6 TLDs at different locations on the terrace Table 5.6 Results of TLD at different locations on the terrace Location

Center

Edge

Corner

Maxm joint accln without TLD

4.945

5.1052

4.8917

Maximum displacement without TLD

0.5252

0.5416

0.5189

Base shear without TLD

37434

37390

35873

Maximum accln with TLD

2.195

2.7593

2.741

Maximum displacement with TLD

0.2979

0.2882

0.2868

Base shear with TLD

22140

22142

22129

% reduction in relative acceleration

55.612

45.951

43.966

% reduction in displacement

43.279

46.787

44.729

% reduction in base shear

40.856

40.781

38.313

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5.0% 4.859 0.548 37999 2.1459 0.2275 16859 55.837 58.485 55.633

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5.7 TLDs for different number of storeys of building Table 5.7 Results for different number of storeys of building Number of storeys

10 storey

15 storey

20 storey

25 storey

35 storey

Maxm accln without TLD

10.044

6.707

5

3.887

2.643

Maxm disp without TLD

0.2318

0.369

0.53

0.712

1.282

Base shear without TLD

39910

38933

37426

35786

34195

Maximum accln with TLD

6.136

4.055

2.38

2.234

1.445

Maxm disp with TLD

0.1367

0.214

0.3055

0.397

0.668

Base shear with TLD

25463

24127

21776

20550

18812

% Reduction in relative accln

38.909

39.541

52.400

42.526

45.327

% Reduction in disp

41.027

42.005

42.358

44.242

47.894

% Reduction in base shear

36.199

38.029

41.816

42.575

44.986

6

DISCUSSION:

Each analysis has been discussed separately under the following headings as given below.

1.

2.

3.

4.

5.

6.

7.

6.1

Standard TLD designed for a G+19 building TLDs at different excitation frequency ratios TLDs with different tuning ratios TLDs with different depth ratios TLDs with different mass ratios TLDs at different locations on the terrace TLDs for different number of storeys of building

Standard TLD designed for a G +19 building

The detailed study done on G+19 building shows that the response of a building for an earthquake can be reduced by as much as 40-50% when the frequency of an earthquake matches with the natural frequency of the building (i.e.: resonance). This conclusion can be drawn from the results obtained by sinusoidal time history analysis.

However, results weren’t as impressive when Response Spectrum analysis was conducted. Response spectrum analysis only showed a reduction by about 20%.

6.2

TLDs at different excitation frequency ratios

Excitation ratio is the ratio of frequency of sinusoidal wave to the fundamental frequency of the building. When the excitation ratio is 1 (i.e.: when the frequency matches), we see resonance and violent shaking of the building. At resonance, the response has magnified by about 5-10 times the normal response. However, when TLD has been introduced to the Š 2018, IRJET

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building, the violent shaking has been stabilized. Although we still see peak values at resonance condition, this peak value is much lesser than the initial peak values. This shows the effectiveness of TLD in controlling earthquake response during resonance condition. However, it is to be noted that the difference TLD is making for response other than resonant response is minimal. This means the TLD has less or no effect for excitations other than the resonating frequencies.

6.3

TLDs with different tuning ratios

Tuning ratio is the ratio of the frequency of the TLD to the frequency of the building. The results show that the best response reduction is obtained when TLD is tuned perfectly to the frequency of the building. The results also show that the deviation in tuning by up to about 5% is acceptable. However, if deviation is beyond 5%, the TLD becomes less effective.

When a TLD is designed, it is to be kept in mind that the added mass of tank would increase the natural time period of the building. So, it is best to design TLD for a tuning ratio of about .97 to .98. Literatures suggest the use of tuning ratio given by: Tuning ratio = 1 / (1+mass_ratio) .....................

The tuning ratio obtained by this method for 2% mass ratio turns out to be .98.

6.4

TLDs with different depth ratios

Depth ratio is the ratio of height of liquid in the tank to the length of liquid in the direction of motion. The ratio of convective mass of liquid to impulsive mass of liquid has an inversely dependent relationship with depth ratio. So, higher depth ratio indicates a lower convective mass, and hence, lesser response reduction during earthquakes. The results presented in this study are in agreement with this statement. As depth ratio has increased, correspondingly, response reduction has also reduced. However, it is to be kept in mind that a lower depth ratio necessitates high number of tanks which may be economically and practically infeasible. Seeing the results from this study, a depth ratio of 0.2 to 0.3 can be recommended.

6.5

TLDs with different mass ratios

Mass ratio is the ratio of mass of liquids in the tank to the mass of the entire structure. The results of analysis conducted in this study shows that the TLD system with higher mass ratio shows a higher reduction in response than a TLD system with a lower mass ratio. This is probably because the force exerted by the water mass depends on the mass of water itself.

However, it is to be kept in mind that a very high mass ratio would necessitate stronger structural design of the building and a very high number of tanks. This may be unfeasible. So, an optimal mass ratio of 2% is recommended by the results of this study.

6.6

TLDs at different locations on the terrace

3 analyses were carried out. One, by placing the TLD in the centre. Two, by placing the TLD at the edge. And three, by placing the TLD at the corner. The reduction in response was found to be maximum when the TLD was placed at the centre. However, the change in response shown by placing TLD in these three locations was very less. This means that the effect of position of TLD on a building has negligible effect in its response. But even so, more preference should be given for a central position.

6.7

TLDs for different number of storeys of building

The analysis was done for buildings with number of storeys varying from 10 to 35. From the results of this analysis, we see that the damping effect of TLD increases with the number of storeys. It is also to be noted that the size of tank increases with the increase in number of storeys. Because of this, lesser number of tanks becomes sufficient to provide the required damping effect. With this study, we find that TLDs are more effective and at the same time, more practical and feasible for taller structures than for shorter ones.

7

CONCLUSIONS

From this study, the following conclusions can be made.  

It has been found that TLD can be successfully modelled in SAP2000 even though there may be many numbers of tanks by using an equivalent spring mass system.

Analyses on TLD showed that TLDs can be effectively used to reduce the response of a structure during earthquakes.

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    

8

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The effect of TLD is found to be significant only in resonance zone. A reduction in response by as much as 45%-50% is obtained when earthquake’s frequency matches building’s natural frequency. In other words, TLD is found to be the most effective in reducing the violent shaking of building during resonance. However, during non-resonance, TLD doesn’t have much effect.

The effect of TLD is found to increase with an increase in mass ratio. The mass ratio for designing TLD was found to be optimal when it is about 2%.

The effect of TLD is found to decrease with an increase in depth ratio. However, with regards to feasibility, a depth ratio of 0.2 to 0.3 is found to be the most optimal.

The effect of tuning ratio is found to be critical in the design of TLD. A deviation in tuning by up to 5% is found acceptable. However, beyond this, a sharp reduction in effectiveness is found out. It is found out that it is best to tune the TLD to 98% of the building’s natural frequency.

The damping effect of TLD is found to be more pronounced for taller buildings with more number of storeys than for shorter buildings.

Furthermore, TLD is also found to be more practical and economical for taller buildings. This is due to the fact that the size of each tank of TLD would be much higher for taller buildings and building such large tanks would be more practical than building many number of small tanks.

REFERENCES 1

Bauer, H. F. (1984). Oscillations of immiscible liquids in a rectangular container: A new damper for excited structures. Journal of Sound and Vibration, 93 (1) pp 117-133.

2

C.G. Koh, S. Mahatma, C.M. Wang. (1995). Reduction of structural vibrations by multiple-mode liquid dampers (Vols. 17 pp. 122-128). Engineering Structures.

3

F. Casciati, A.D. Stefano, E. Matta. (2003). Simulating a conical tuned liquid damper (Vols. 11 pp. 353-370).

Simulation Modelling Practice and Theory.

4

Housner G. W. (1963). The Dynamic Behaviour of Water Tanks. Bulletin of the Seismological Societyof America, 53.

5

K. Fujii, Y. Tamura, T. Sato, T. Wakahara. (1990). Wind-induced vibration of tower and practical applications of Tuned Sloshing Damper. (Vols. 33, pp. 263-272). Journal of Wind Engineering and Industrial Aerodynamics.

6

Kim Y.M., You K.P., Cho J.E., Hong D.P. (2006). The Vibration Performance Experiment of Tuned Liquid Damper and Tuned Liquid Column Damper (Vols. 20 pp.795-805). Journal of Mechanical Science and Technology.

7

L.M. Sun, Y. Fujino, B.M.Pacheco , and P. Chaiseri. (1992). Modeling of Tuned Liquid Damper (TLD). Journal of Wind Engineering and Industrial Aerodynamics, 41-44, pp. 18831894.

8

M.J. Tait. (2008). Modelling and preliminary design of a structure -TLD system (Vols. 30 pp. 2644-2655).

Engineering Structures.

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N.S. Sebastian, D. A. (2017). Seismic Analysis of Elevated Water Tank in a Framed Building. International Research Journal of Engineering and Technology (IRJET), 4(6).

10 Novo T., Varum H., Teixeira-Dias F., Rodrigues H., Falcao Silva M., Campos Costa A. and Guerreiro L. (2013). Tuned Liquid Dampers Simulation for Earthquake Response control of Buildings. Bulletin of Earthquake Engineering.

11 Samanta A., Banerji P. (2008). Structural Control Using Modified Tuned Liquid Dampers. 14th World Conference on Earthquake Engineering, China.

12 Shang C.Y., Zhao J.C. (2008). Periods and Energy Dissipations of a Novel TLD Rectangular Tank with Angleadjustable Baffles (Vols. 13 pp. 139-141). J. Shanghai Jiaotong University.

13 Soong, T., & Dargush, G. F. (1997). Passive Energy Dissipation Systems in Structural Engineering. . UK: John Wiley & Sons Ltd. 14 Soong, T.T; Dargush, Gary F. (1997). Passive Energy Dissipation Systems in Structural Engineering. UK: John Wiley & Sons Ltd. © 2018, IRJET

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15 T. Balendra, C. W. (2001). Control of wind-excited towers by active tuned liquid column damper (Vol. 23 pp.10541067). Engineering Structures .

16 T. Novo, H. Varum, F. Teixeira-Dias, H. Rodrigues, M. Falcao Silva, A. Campos Costa, L. Guerreiro. (2013). Tuned Liquid Dampers Simulation for Earthquake Response control of Buildings (Vols. 10.1007/s10518-013-9528-2).

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17 V.J. Modi, A. Akinturk. (2002). An efficient liquid sloshing damper for control of wind-induced instabilities (Vol. 90 pp. 19071918). Journal of wind engineering and industrial aerodynamics.

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19 X.L. Xu, K.C.S. Kwok, B. Samali. (1992). The effect of tuned mass dampers and liquid dampers on cross-wind response of tall/slender structures (Vols. 40 pp. 33-54). Journal of Wind Engineering and Industrial Aerodynamics.

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